| Identifier | .dat | .fil | .odb | Description |
| Field | History |
| All analysis types |
| SOAREA | ● | ● | | ● | Area of the defined section. |
| Stress/displacement analysis |
| SOF | ● | ● | | ● | Total force in the section. |
| SOM | ● | ● | | ● | Total moment in the section. |
| SOCF | ● | ● | | ● | Center of the total force in the section. |
| Heat transfer analysis |
| SOH | ● | ● | | ● | Total heat flux associated with the section. |
| Electrical analysis |
| SOE | ● | ● | | ● | Total current associated with the section. |
| Mass diffusion analysis |
| SOD | ● | ● | | ● | Total mass flow associated with the section. |
| Coupled pore fluid diffusion-stress analysis |
| SOP | ● | ● | | ● | Total pore fluid volume flux associated with the section. |
# Whole and partial model variables
The output variables listed below are available for part of the model as well as the whole model.
Identifier .dat .fil .odb Description Field History
# Adaptive mesh domains
The following variable is available only for adaptive domains (see “Defining ALE adaptive mesh domains in Abaqus/Standard,” Section 12.2.6).
VOLC Change in area or change in volume of an element set solely due to adaptive meshing.
# Equivalent rigid body motion variables
You can request equivalent rigid body motion whole element set variable output to the data, results, or output database file (see “Element output” in “Output to the data and results files,” Section 4.1.2, and
Identifier .dat .fil .odb Description Field History
“Element output” in “Output to the output database,” Section 4.1.3). The variables listed are available only for implicit dynamic analyses using direct integration except where indicated.
| XC | • | • | • | Current coordinates of the center of mass for the entire set or the entire model. Not available for eigenfrequency extraction, eigenvalue buckling prediction, complex eigenfrequency extraction, or linear dynamics procedures. Available also for static analyses but only from the output database. |
| XCn | • | | • | Coordinate n of the center of mass for the entire set or the entire model (n = 1, 2, 3). |
| UC | • | • | • | Current displacement of the center of mass for the entire set or the entire model. Available also for static analyses but only from the output database. |
| UCn | • | | • | Displacement component n of the center of mass for the entire set or the entire model (n = 1, 2, 3). |
| URCn | • | | • | Rotation component n of the center of mass for the entire set or the entire model (n = 1, 2, 3). |
| VC | • | • | • | Equivalent rigid body velocity components summed over the entire set or the entire model. |
| VCn | • | | • | Component n of the equivalent rigid body velocity summed over the entire set or the entire model (n = 1, 2, 3). |
| VRCn | • | | • | Component n of the equivalent rigid body angular velocity summed over the entire set or the entire model (n = 1, 2, 3). |
| HC | • | • | • | Current angular momentum about the center of mass for the entire set or the entire model. |
| HCn | • | | • | Component n of the angular momentum about the center of mass for the entire set or the entire model (n = 1, 2, 3). |
| HO | • | • | • | Current angular momentum about the origin for the entire set or the entire model. |
| HOn | • | | • | Component n of the angular momentum about the origin for the entire set or the entire model (n = 1, 2, 3). |
| RI | • | • | • | Current rotary inertia about the origin of the entire set or the entire model. Not available for eigenfrequency |
| IRX | • | • | Current coordinates of the reference point. |
| IRXn | • | • | Coordinate n of the reference point (n = 1, 2, 3). |
| IRA | • | • | Equivalent rigid body acceleration components. |
| IRAn | • | • | Component n of the equivalent rigid body acceleration (n = 1, 2, 3). |
| IRARn | • | • | Component n of the equivalent rigid body angular acceleration with respect to the reference point (n = 1, 2, 3). |
| IRF | • | • | Inertia relief load corresponding to the equivalent rigid body acceleration. |
| IRFn | • | • | Component n of the inertia relief load corresponding to the equivalent rigid body acceleration (n = 1, 2, 3). |
| IRMn | • | • | Component n of the inertia relief moment corresponding to the equivalent rigid body angular acceleration with respect to the reference point (n = 1, 2, 3). |
| EIGVAL | ○ | ○ | Eigenvalues. |
| EIGFREQ | ○ | ○ | Eigenfrequencies. |
| GM | ○ | ○ | Generalized masses. |
| CD | ○ | ○ | Composite damping factors. |
| PFn | ○ | ○ | Modal participation factors 1–7 (n = 1,2,3 corresponding to displacements, n = 4,5,6 for the rotations, and n = 7 for acoustic pressure). |
| EMn | ○ | ○ | Modal effective masses 1–7 (n = 1,2,3 corresponding to displacements, n = 4,5,6 for the rotations, and n = 7 for acoustic pressure). |
Identifier .dat .fil .odb Description
# Field History
# Complex eigenvalue extraction
The following variables are output automatically during a complex frequency extraction analysis (“Complex eigenvalue extraction,” Section 6.3.6).
| Identifier | .dat | .fil | .odb | Description |
| Field | History |
| ALLCCSDT | ○ | | | ● | Contact constraint stabilization dissipation in tangential direction. |
| ALLCCSD | ○ | | | ● | The sum of ALLCCSDN and ALLCCSDT. |
| ALLCD | ○ | ○ | | ● | Energy dissipated by creep, swelling, viscoelasticity, and energy associated with viscous regularization for cohesive elements and cohesive contact. |
| ALLEE | ○ | ○ | | ● | Electrostatic energy. |
| ALLFD | ○ | ○ | | ● | Total energy dissipated through frictional effects. (Available only for the whole model.) |
| ALLIE | ○ | ○ | | ● | Total strain energy. (ALLIE = ALLSE + ALLPD + ALLCD + ALLAE + ALLQB + ALLEE + ALLDMD.) |
| ALLJD | ○ | ○ | | ● | Electrical energy dissipated due to flow of electrical current. |
| ALLKE | ○ | ○ | | ● | Kinetic energy. In steady-state dynamic analysis this is the cyclic mean value. |
| ALLKL | ○ | ○ | | ● | Loss of kinetic energy at impact. (Available only for the whole model.) |
| ALLPD | ○ | ○ | | ● | Energy dissipated by rate-independent and rate-dependent plastic deformation. |
| ALLQB | ○ | ○ | | ● | Energy dissipated through quiet boundaries (infinite elements). (Available only for the whole model.) |
| ALLSD | ○ | ○ | | ● | Energy dissipated by automatic stabilization. This includes both volumetric static stabilization and automatic approach of contact pairs (the latter part included only for the whole model). |
| ALLSE | ○ | ○ | | ● | Recoverable strain energy. In steady-state dynamic analysis this is the cyclic mean value. |
| ALLVD | ○ | ○ | | ● | Energy dissipated by viscous effects including viscous regularization (except for cohesive elements and cohesive contact), not inclusive of energy dissipated by automatic stabilization and viscoelasticity. |
| ALLDMD | ○ | ○ | | ● | Energy dissipated by damage. |
| ALLWK | ○ | ○ | | ● | External work. (Available only for the whole model.) |
| ETOTAL | ○ | ○ | | ● | Total energy balance (available only for the whole model). (ETOTAL = ALLKE + ALLIE + ALLVD + ALLSD + ALLKL + ALLFD + ALLJD + ALLCCE - ALLWK - ALLCCDW.) |
# Solution-dependent amplitude variables
Solution-dependent amplitude variables are given automatically with any file output or output database request.